An isothermal cooking plate assembly is formed from a first plate of high thermal conductivity material having a back surface and an oppositely disposed top cooking surface. One or more heater circuit assemblies are disposed on the first plate back surface for forming a composite having a back surface. A controller is in electrical connection with the heater circuit assemblies for controlling temperature of the first plate of high thermal conductivity material. The first plate can be Aluminum Type 1100 or Aluminum Type 6061. The first plate can be a laminate formed from a clad bottom metal layer and clad top cooking surface metal layer, where the clad layers formed from the same material and having about the same thickness. The clad material can be austenitic stainless steel. A second plate of low thermal conductivity material can be attached to the composite back surface of first plate.
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1. An isothermal cooking plate assembly (50) mechanically attached within a griddle system (10) and comprising:
(a) a first plate (52) of high thermal conductivity material comprising aluminum whose thickness is substantially uniform, having a thermal conductivity of at least 1.67 watts/cm-c, a surface area of not greater than 54 square inches, a length-to-width aspect ratio that does not exceed about 1.5, a thickness in the range of 0.187 to 0.250 inches, and having a back surface (159) and an oppositely disposed top food-cooking surface (28);
(b) a thick-film printed and fired heater circuit assembly (130) disposed on and substantially covering the first plate back surface (159) and comprising:
(i) a first glass thick-film printed and fired electrically insulative layer (141) disposed on the first plate back surface (159) having a thickness that does not exceed a maximum allowed thickness, tdielectric of the glass thick-film printed and fired first electrically insulative layer, the maximum allowed thickness, tdielectric #30# corresponding to the maximum allowable thickness of the first electrically insulative layer that avoids the fracture, cracking and/or breaking of the thick-film printed and fired first electrically insulative layer during rapid heat-up of the aluminum first plate, the maximum allowed thickness, tdielectric calculated using the equation (Equation 1H):
tdielectric=[{σdielectric*(1−μ)}/{αdielectric*Edielectric}]*[kdielectric/{Qheater/Aheater}], wherein the calculated maximum allowed value for the thickness, tdielectric Of the glass thick-film printed and fired first electrically insulative layer is based on maximum level of applied heat flux, {Qheater/Aheater} and known thermal conductivity, kdielectric of the glass thick-film printed and fired first electrically insulative layer as well as the known properties of glass including the breaking strength of glass, σdielectric; modulus of elasticity, Edielectric coefficient of thermal expansion, αdielectric and Poisson's ratio, μ;
(ii) third electrically conductive bus strips (132a and 132b) thick film printed onto the previously thick-film printed and fired first surface of first electrically insulative layer;
(iii) second electrically resistive heating element legs (144a-144r and 145) thick-film printed and fired on previously thick-film printed and fired first surface of first electrically insulative layer and extending onto the previously thick-film printed and fired third electrically conductive bus strips to effect electrical communication between the second electrically resistive heating element legs and the third electrically conductive bus strips; and
(iv) distal ends of first and second electrical leads (158, 160) removably attachable to first and second contact pads (62, 64), respectively, wherein the first and second electrical contact pads are disposed on the third electrically conductive bus strips; and
(c) a controller (20) in electrical communication with the thick-film printed and fired heater circuit assembly through removably attachable first and second electrical leads (158, 160) at first and second contact pads (62, 64), respectively, on the third electrically conductive bus strips, controlling a temperature of the first plate top food-cooking surface using temperature sensor (39) removably attached to first plate;
the first plate, thick-film printed and fired heater circuit assembly and a second plate (30) combine to form cooking plate assembly (50) wherein:
(i) the maximum temperature difference between an operator selected set point temperature and any temperature of the first plate top food-cooking surface in contact with food is less than about 10 c for set point temperatures up to about 230 c, and
(ii) the rate of heat-up of the first plate from about 25 c to about 150 c is less than about 30 seconds using an applied voltage of 115 volts and maximum current of 20 amps for the single heating circuit assembly substantially covering the first plate back surface.
2. The isothermal cooking plate assembly of
3. The isothermal cooking plate assembly of
4. The isothermal cooking plate assembly of
5. The isothermal cooking plate assembly of
6. The isothermal cooking plate assembly of
7. The isothermal cooking plate assembly of
8. The isothermal cooking plate assembly of
9. The isothermal cooking plate assembly of
10. The isothermal cooking plate assembly of
11. An array of two or more of the isothermal laminate cooking plate assemblies of
12. The isothermal cooking plate assembly of
(T′1 #30# −T′2)max={σdielectric(1−μ)}/{αdielectric*Edielectric}. 13. The isothermal cooking plate assembly of
14. The method of manufacturing an isothermal cooking plate assembly comprising the steps of:
(a) providing a first plate comprising aluminum whose thickness is substantially uniform, having a thermal conductivity of at least 1.67 watts/cm-c, a surface area of not greater than 54 square inches, a length-to-width aspect ratio that does not exceed about 1.5, a thickness in the range of 0.187 to 0.250 inches, and having a back surface and an oppositely disposed top food-cooking surface;
(b) depositing a thick-film printed and fired heater circuit assembly on and substantially covering the first plate back surface comprising the steps of:
(i) thick film printing and firing a glass thick-film printed and fired electrically insulative layer on the first plate back surface, the glass thick-film printed and fired electrically insulative layer having a thickness that does not exceed a maximum allowed thickness, tdielectric of the glass thick-film printed and fired first electrically insulative layer which avoids fracture, cracking and/or breaking of the thick-film printed and fired first electrically insulative layer during rapid heat-up of the aluminum first plate, the maximum allowed thickness, tdielectric calculated using the equation the following equation (Equation 1H):
tdielectric=[{σdielectric*(1−μ)}/{αdielectric*Edielectric}]*[kdielectric/{Qheater #30# /Aheater}], wherein the calculated maximum allowed value for the thickness, tdielectric of the glass thick-film printed and fired first electrically insulative layer is based on maximum level of applied heat flux, {Qheater/Aheater} and known thermal conductivity, kdielectric of the glass thick-film printed and fired first electrically insulative layer as well as the known properties of glass including the breaking strength of glass, σdielectric; modulus of elasticity, Edielectric coefficient of thermal expansion, αdielectric and Poisson's ratio, μ;
(ii) thick film printing and firing an electrically conductive bus strip in electrical communication with the electrically resistive heating element legs and mechanically connectable to and in electrical communication with the first and second electrical leads;
(iii) thick film printing and firing second an electrically resistive heating element legs disposed on the electrically insulative layer;
(iv) thick film printing and firing an electrically insulative cover layer over the electrically conductive bus strips except at locations of contact pads as well as over the electrically resistive heating element legs; and
(c) mechanically attaching a second plate of low thermal conductivity material to the back surface of the first plate of high thermal conductivity material and oppositely disposed to the top food-cooking surface.
15. The method of
16. The method of
17. The method of
18. The method of
19. The method of
20. The method of
21. The method of
22. The method of
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This application is a continuation-in-part of application Ser. No. 16/044,774 filed Jul. 25, 2018, now U.S. Pat. No. 10,995,959, which in turn is a continuation-in-part of application Ser. No. 14/526,570 filed Oct. 29, 2014, now abandoned, which claims benefit of provisional application Ser. No. 61/899,415 filed on Nov. 4, 2013; the disclosures of which are expressly incorporated herein by reference.
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The accurate temperature control of cooking plate assemblies, also known as griddles, is required for certain food processing wherein variable rates of heat dissipation exist across the extent of the cooking surface. Some applications would benefit from improved energy efficiency if the cooking surfaces could be raised from room temperature to the desired operating temperature within a very brief time period so that the cooking plate (or griddle) is only heated during the time period that the cooking of food is required. Furthermore, some applications require that the cooking plate assembly be suitable and safe for contact with objects, such as liquid or solid foods, and be resistant to damage by exposure to liquids and mechanical damage by contacting objects such as knives and other cooking implements. In addition, there is a need to provide a cooking surface comprising a non-stick coating to minimize the need for supplemental cooking liquids (e.g., cooking oils) and minimize the effort required to clean adhered food residue from the cooking surface following prior cooking processes.
Accordingly, there is a need to provide a durable cooking plate capable of delivering and thermally conducting a sufficient amount of heat to maintain a substantially uniform or isothermal temperature distribution across the extent of the cooking plate surface while maintaining a pre-selected temperature in the presence of rapidly and widely varying heat dissipation rates across the surface of the cooking plate. The need for an isothermal cooking plate assembly capable of maintaining a substantially uniform temperature is a critical food safety requirement to ensure the adequate cooking of meat and poultry (e.g., steak, ground meat, ground poultry, hamburger patty, sausage patty) since cooking for a predetermined time interval (i.e., “cook by time”) for a given type of food and food article is widely used in fast-food kitchens, food trucks (i.e., trucks that contain mobile kitchens to prepare food at multiple customer walk-up sites) and hotel/motel hospitality food services. In this regard, an operator that typically has limited professional cooking skills utilizes a settable elapsed time device (i.e., timer) to determine when the food article being cooked on the griddle is either ready to be cooked on opposite uncooked side or that the food article is adequately cook to ensure the safe consumption of the food. Limiting the maximum difference between the operator-selected temperature and any region of the cooking plate in contact with food to 10 C. or less for the full range of cooking plate loading factors (i.e., fraction of cooking plate covered by food) and operator-selectable set-point temperatures up to 230 C (450 F) enables food to be cooked safely and consistently once the cooking duration parameter is initially confirmed through the simple measurement of the minimum internal temperature of the article of food using widely available meat thermometers. Once the required cooking duration is determined (using thermometry) that ensures that the minimum internal temperature of the food is cooked to an established safe temperature (e.g., 160 F or 71 C for the case of hamburger), then that determined cooking duration (e.g., 500 seconds) can be used in subsequent cooking of the same type and size of food article as long as the food cooking plate is known to be substantially equal to the operator selected set point (i.e., within 10 C or less of the operator selected set-point temperature).
A griddle system that incorporates an isothermal cooking plate assembly requiring only a brief period to heat up the first plate cooking surface from room temperature to an operator-selected set-point temperature, preferably within 30 seconds, is also needed since many applications involve “on demand” cooking of food, i.e., cooking of food when an individual order is received such as cooking food on a food truck or in the kitchen of a hotel/motel hospitality breakfast service. The ability to heat up the first plate of an isothermal cooking plate assembly of a griddle system within 30 seconds results in a significant savings of power and reduces environmental cooling requirements since the isothermal cooking plate assembly is heated to a cooking temperature (e.g., 150 C) for only the period of time during which the cooking of one or more articles of food is actually being performed. As a result, the ability to heat up the first plate of an isothermal cooking plate assembly of a griddle system within 30 seconds provides: [a] a reduction in the operator's food preparation time for a given food cooking request, [b] an increase in the number of customers that can be served per unit time (e.g., customers served per hour) and [c] a reduction in the cost for energy required for cooking food since electrical power is only being supplied to the isothermal cooking plate assembly of the griddle system at the time a request for cooked food is received (e.g., an food order is received for a cooked hamburger).
A griddle system that incorporates an isothermal cooking plate assembly requiring a source of electrical power having a voltage of only 115 volts at a maximum current of 20 amps is also needed since it would be useful in many settings such as hospitality food service kitchens of hotels and motels as well as food trucks and “mom and pop” short order kitchens that prepare food on demand (i.e., as orders are received). This capability eliminates the need for a special high-voltage 220-volt service installation that requires specially wiring within the walls or a custom external conduit to extends to a special high-voltage outlet and a special addition to the utility box to accommodate each dedicated 220-volt outlet.
In addition, there is a need to simplify the complexity of the cooking plate construction to increase its reliability and reduce its manufacturing costs to enable its use in high-volume cooking applications and enable rapid and convenient replacement of only the cooking plate assembly in the event of deterioration and loss of release characteristics of the non-stick coating, failure of the electrically resistive heating element and/or failure of temperature sensor without the need for replacing the cooking plate support structure, partial enclosure or temperature control electronics comprising the controller, temperature sensor, and power leads to the electrically resistive heating element.
An example embodiment of the present disclosure is a griddle system incorporating two independently controlled isothermal cooking plate assemblies. It is estimated that the total manufacturing cost for a griddle system having two independently controllable cooking stations is less than $1,000. At this manufacturing cost level, the finished product could be sold at a price level that could be accommodated by a wide range of food service operators including hospitality food service kitchens of hotels and motels as well as food trucks and “mom and pop” short order kitchens that prepare food on demand. In addition, the estimated cost for each independently controllable and readily replaceable isothermal cooking plate assembly is less than $200.
The present disclosure is addressed to design for a griddle system comprising an isothermal cooking plate assembly, controller, griddle system and method of manufacture of the isothermal cooking plate assembly. As described more fully below, the present disclosure specifies the optimum design for a griddle system wherein one or more independently controlled isothermal cooking plate assemblies are optimized for [a] a maximum temperature difference between the operator-selected set-point temperature and any temperature within cooking plate in contact with food that does not exceed the set-point temperature by more than 10 C for all set-point temperatures, [b] a rapid heat-up from room temperature to the operator-selected set-point temperature of less than 30 seconds, [c] convenient use of readily available line power at a maximum current of 20 amps at 115 volts (i.e., standard capacity of most electrical outlets) and [d] convenient replacement of a low-cost isothermal cooking plate assembly in the field (e.g., replacement due to degradation over time of the non-stick coating or failure of the heating element) while reusing the griddle controller and support structure. The isothermal cooking plate assembly includes a first plate of high thermal conductivity material that advantageously may be Aluminum Type 1100 or Type 6061. The preferred material for first plate is Aluminum Type 1100 owing to its higher thermal conductivity of 2.18 watts/cm-C as compared Aluminum Type 6061 having a thermal conductivity of 1.67 watts/cm-C. The first plate has a substantially uniform thickness over the full extent of its surface used for cooking.
As used herein, the term “substantially uniform thickness” refers to the standard thickness tolerance for commercially available materials in the form of sheets. By way of example, Aluminum 1100 sheet stock is available from McMaster Carr (Cleveland, Ohio) in sheet sizes up to 48 inch×96 inch having a thickness of 0.190 inch and a thickness tolerance of +/−0.011 inch. At a sheet thickness of 0.250 inch, Aluminum 1100 sheet stock is available from McMaster Carr (Cleveland, Ohio) in sheet sizes up to 48 inch×96 inch having a thickness tolerance of +/−0.016 inch.
Based on the detailed heat transfer analyses performed as well as the calculation of heat up rates of alternative first plates of isothermal cooking plate assemblies, the commercially available thickness tolerances are sufficiently small that the computed temperature distributions of the first plate as well as the calculated rates of heat-up to the set-point temperature (e.g., 150 C) are effectively unchanged. For example, for an Aluminum 1100 first plate having a length of 7.9 inch and a width of 6.3 inch, the time required to heat up from 25 C to 150 C at a specified thickness of 0.187 inch and maximum power input of 115 volts at 20 amps (i.e., 2300 watts) is 20.8 seconds. If the Aluminum 1100 sheet having a nominal thickness of 0.187 inch is manufactured at the maximum commercially available thickness based on a thickness tolerance of +/−0.011 inch, then the heat up time for the maximum manufactured sheet thickness of 0.187 inch+0.011 inch or 0.198 inch is 22.0 seconds or 1.2 seconds longer than the heat up time for the first plate having a nominal sheet thickness of 0.187 inch.
The uniformly thick first plate of high thermal conductivity material may optionally be roll bonded on top cooking surface of first plate with a cladding layer, for instance, formed of austenitic stainless steel, such as a Type 304 and having a thickness of 0.002 to 0.010 inch. The corrosion-resistant and durable cladding (e.g., austenitic stainless steel) may be applied by roll bonding, plasma spray coating or vapor deposition processes. In addition, the hardness, wear resistance, corrosion resistance, and lubricity of the exterior surface of the stainless steel cladding may be further improved using metal finishing processes such as MEDCOAT 2000™ provided by the Electrolyzing Corporation of Ohio (Cleveland, Ohio). Alternatively, the cooking surface of the first plate of high thermal conductivity material may coated with a corrosion resistant and durable surface layer applied by electroplating or electroless plating processes (e.g., nickel or chrome plated surface coating).
A non-stick coating may be advantageously disposed on and in good thermal communication with the top cooking surface of the first plate of high thermal conductivity material of the present disclosure to minimize the need for supplemental cooking liquids (e.g., cooking oils) and to minimize the effort required to clean adhered food residue from the top cooking surface following prior cooking processes. If a non-stick coating is disposed on and in good thermal communication with the top cooking surface of the first plate, its application and curing would occur only after all of the thick-film printing and firing steps for the first electrically insulative layer, second electrically resistive heating element, third electrically conductive bus strips, and optional fourth electrically insulative covering layer, as specified below.
As used herein, the term “firing” of glass-based, thick-film printed layers refers to an elevated-temperature process that functions to remove any residual organic carriers from the printed thick-film layer and during which the printed thick-film layer is bonded to its underlying substrate. For the case of thick-film layers containing electrically conducting particles or electrically resistive glass particles, the firing process enables the development of the intended electrically conductive or electrically resistive properties of the thick-film layer as a result of the coalescence of the filler particles.
A heater manufacturing method involves a first plate of thermally conductive material that is metallic on which is disposed one or more thick-film printable first electrically insulative layers incorporating a glass having a large coefficient of thermal expansion that can be thick-film printed on the back surface of the first plate opposite its top cooking surface. Each thick-film printable, glass-based first electrically insulative layer is then fired at a temperature, Tdielectric that does not exceed the melting point of first aluminum plate, preferably fired at a temperature, Tdielectric that does not exceed 600 C.
Following the firing of one or more thick-film printable first electrically insulative layers, two or more silver-filled, glass-based third electrically conductive bus strips are thick film printed onto the previously thick-film printed and fired first surface of the first electrically insulative layer, preferably oppositely disposed at the edges of the first plate to provide for electrical connections to the electrically resistive heating element legs as well as contact pads for electrical communication between the second electrically resistive heating element and removably attachable electrical leads extending from controller. The thick-film printed third electrically conductive bus strips are then fired at a temperature, Tbus-strip, that is lower than the temperature at which the thick-film printable first electrically insulative layer is fired, Tdielectric, in order to prevent migration of the third electrically conductive bus strips into the previously fired first electrically insulative layer in order to prevent an unwanted electrical conduction path between the third electrically conductive bus strips and the first plate. Preferably, the firing temperature for the thick-film printable third electrically conductive bus strips, Tbus-strip is at least 50 C lower than the temperature at which the thick-film printable first electrically insulative layer is fired, Tdielectric.
Following the firing of two or more thick-film printable third electrically conductive bus strips, a second electrically resistive heating element layer incorporating glass that contains electrically conductive fillers is thick-film printed and fired on the previously thick-film printed and fired first surface of the fired first electrically insulative layer as well as extending onto the previously thick-film printed and fired electrically conductive bus strips to effect electrical communication between the second electrically resistive heating element layer legs and the electrically conductive bus strips. The second electrically resistive heating element layer then is fired at a temperature, Theater, that is lower than the temperature at which the two or more thick-film printable thick-film printable electrically conductive bus strips, Tbus-strip are fired. Preferably, the firing temperature for the thick-film printable second electrically resistive heating element layer, Theater is at least 50 C lower than the firing temperature at which the thick-film printable electrically conductive bus strips, Tbus-strip. In addition, an optional fourth electrically insulative covering layer may be deposited over the second electrically resistive heating element layer and the third electrically conductive bus strips.
By way of example, the firing temperatures for first electrically insulative layer, Tdielectric, third electrically conductive bus strips, Tbus-strip and second electrically resistive heating element layer, Theater may be 550 C, 500 C and 450 C, respectively. In this manner, each successive firing temperature is sufficiently below the firing temperature used for the preceding layer that there is no migration of thick-film constituents into previously fired layers.
The thick-film printed and fired first electrically insulative layer of the present invention is an inorganic glass or glass-ceramic dielectric comprising a mixture of two or more oxides and exhibiting a large coefficient of thermal expansion, αdielectric comparable to the coefficient of thermal expansion of aluminum, αaluminum (viz., 21×10−6 per degree C.). In this regard see Wilder, J. A., Glass Ceramics for Sealing to High Expansion Metals. Sandia National Laboratories 1980; Report No. SAND80-2192: 1-26. In this regard, also see U.S. Pat. Nos. 5,262,364 and 9,776,911.
In addition, the thick-film printed first electrically insulative layer of the present invention, following firing, can be further characterized by the measurable mechanical and thermal properties that include the fired material's [a] modulus of elasticity, Edielectric, [b] thermal conductivity, kdielectric and [c] breaking strength of glass, αdielectric. As used herein, the breaking strength of glass refers to the measured and reported level of stress at which glass will fracture, crack or break.
As specified in the present invention, the thick-film printed and fired first electrically insulative layer provides the dual functions of [a] electrically isolating the second electrically resistive heating element legs and the third electrically conductive bus strips from the aluminum electrically and thermally conductive first plate and [b] thermally conducting heat generated within and from the second electrically resistive heating element legs to the aluminum electrically and thermally conductive first plate. The thick-film printed and fired first electrically insulative layer comprises a first surface at its interface with the thick-film printed and fired electrically resistive heating element legs. The thick-film printed and fired first electrically insulative layer comprises a second surface at its interface with the back surface of the first plate that is opposite the top cooking surface of the first plate. The first surface and second surface of the thick-film printed and fired first electrically insulative layer are separated by a distance, tdielectric that corresponds to the substantially uniform physical thickness of the thick-film printed and fired first electrically insulative layer.
For the general case of heat conduction through a solid having a substantially uniform thickness, t (In units of centimeters), the amount of heat conducted, Q (in units of watts) through an area, A (in units of square centimeters) is proportional to the thermal conductivity, k (in units of watts/sq·cm.-C) of the solid and the temperature difference (T1-T2) across the thickness of the solid (in units of Centigrade degrees). The general equation for heat conduction through a solid having a substantially uniform thickness is provided below in Equation 1:
Q={k*A*(T1−T2)}/t (Equation 1)
In this regard, see McAdams, W. H., Heat Transmission. 1954; McGraw-Hill Book Company, New York: page 12, Equation 2-6.
For the specific case of heat conduction through the thick-film printed and fired first electrically insulative layer of the present invention and based on the well-known heat conduction equation specified above in Equation 1, the amount of heat conducted through the thick-film printed and fired first electrically insulative layer, Qheater is provided below in Equation 1A:
Qheater={kdielectric*Aheater*(T1′−T2′)}/tdielectric (Equation 1A)
The term for the area through which heat is conducted, Aheater corresponds to the total area of the second electrically resistive heating element legs in direct thermal contact with the thick-film printed and fired first electrically insulative layer. The temperatures, T1′ and T2′ in Equation 1A correspond to the temperatures at the first surface and second surface of the electrically insulative layer, respectively.
For the specific case of heat conduction through the thick-film printed and fired first electrically insulative layer of the present invention, the resulting temperature difference, (T1′−T2′) across the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer can be expressed in terms of the amount of heat conducted through the through the thick-film printed and fired first electrically insulative layer, Qheater as well as the area through which heat is conducted, Aheater, the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer and the thermal conductivity, kdielectric of the thick-film printed and fired first electrically insulative layer as specified below in Equation 1B:
(T1′−T2′)={Qheater/Aheater}*{tdielectric/kdielectric} (Equation 1B)
As seen in Equation 1B, the larger the ratio, {Qheater/Aheater}, also referred to hereinafter as the heat flux through the thick-film printed and fired first electrically insulative layer, the larger the resulting temperature difference, (T1′−T2′) across the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer. Likewise, as seen in Equation 1B, the larger the ratio, {tdielectric/kdielectric}, the larger the resulting temperature difference, (T1′−T2′) across the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer. As used herein, “heat flux” refers to the amount of resistive heating (i.e., Joulean heating) generated within the second electrically resistive heating element legs (e.g., in units of watts) divided by the total surface area of the electrically resistive heating element legs disposed on the first electrically insulative layer (e.g., in units of square centimeters or cm2).
The functional significance of Equation 1B for the specific case of heat conduction through the thick-film printed and fired first electrically insulative layer of the present invention is apparent when the breaking strength of the glass thick-film printed and fired first electrically insulative layer, σdielectric is quantified. As used herein, the breaking strength of the glass thick-film printed and fired first electrically insulative layer, σdielectric refers to the applied stress at failure of the glass layer, i.e., the physical fracture, cracking and/or breaking apart of the first electrically insulative layer and its overlaying second electrically resistive heater layer and/or third electrically conductive bus strip layer.
In general, the thermal stress, σ (in units of pounds per square inch) induced in a layer of material having a uniform thickness and that is exposed to a temperature difference, (T1−T2) in units of Centigrade degrees can be expressed by the following equation:
σ={α*E*(T1−T2)}/(1−μ) (Equation 1C)
where α is the coefficient of thermal expansion of the material (in units of reciprocal degrees Centigrade), E is the modulus of elasticity or Young's modulus of the material (in units of pounds per square inch) and μ is Poisson's ratio for the material defined as the ratio of the change in the width per unit width of a material, to the change in its length per unit length, as a result of strain. In this regards, see Young, W. C and Budynas, R. G., Roark's Formulas for Stress and Strain. Seventh Edition 2002; McGraw-Hill Company, New York; Chapter 16.6 Thermal Stresses, page 758-764.
The general equation for thermal stress, σ in a material, as seen in Equation 1 C, can be rearranged to express the temperature difference, (T1−T2) as a function of the thermal stress, σ as well as the coefficient of thermal expansion, α, modulus of elasticity, E and Poisson's ratio, μ, as follows:
(T1−T2)={σ*(1−μ)}/{α*E} (Equation 1D)
Referring to Equation 1D, if the thermal stress, σ is replaced with the breaking strength of the glass thick-film printed and fired first electrically insulative layer, σdielectric (corresponding to the applied stress, σ at mechanical failure of the glass thick-film printed and fired first electrically insulative layer), then Equation 1D expresses the maximum allowable temperature difference, (T′1-T′2)max to avoid mechanical failure (e.g., fracture, cracking, breaking) of the glass thick-film printed and fired first electrically insulative layer as expressed below in Equation 1E:
(T′1−T′2)max={σdielectric*(1−μ)}/{αdielectric*Edielectric} (Equation 1E)
where the temperatures, T1′ and T2′ in Equation 1E correspond to the temperatures at the first surface and second surface of the electrically insulative layer, respectively and the terms αdielectric, Edielectric and μ are as defined in the preceding paragraphs. The maximum allowable temperature difference, (T′1−T′2)max in Equation 1E is equivalent to and referred to hereinafter as the “Maximum Allowable Thermal Stress in the First Electrically Insulative Layer”.
Combining the temperature difference, (T′1−T′2) associated with heat conduction through the glass thick-film printed and fired first electrically insulative layer of the present invention, as seen in Equation 1B with the above expression for the maximum allowable temperature difference, (T′1−T′2)max seen in Equation 1E provides an expression for the “Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer” as specified in Equation 1E. Since both Equation 1B and Equation 1E are equal to the same temperature difference, (T′1−T′2), then, by identity, Equation 1B and Equation 1E can be combined a specified in Equation 1F:
{Qheater/Aheater}*{tdielectric/kdielectric}={σdielectric*(1−μ)}/{σdielectric*Edielectric} (Equation 1F)
The term {Qheater/Aheater}*{tdielectric/kdielectric} refers to the “Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer” that can be induced in the thick-film printed and fired glass first electrically insulative layer without inducing fracture, cracking and/or breaking of the first electrically insulative layer and associated failure of the thick-film printed and fired heater circuit assembly. As seen in Equation 1F, for a given maximum heat flux, Qheater/Aheater through the glass thick-film printed as well as the thickness, tdielectric and thermal conductivity, kdielectric of the fired first electrically insulative layer, the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer corresponding expressed by the term {Qheater/Aheater}*{tdielectric/kdielectric} can be equated to the term {σdielectric*(1−μ)}/{αdielectric*Edielectric}.
Hence, based on the published (nominal) values for the breaking strength of the glass thick-film printed and fired first electrically insulative layer, σdielectric as well as the nominal values for the coefficient of thermal expansion, αdielectric, modulus of elasticity, Edielectric and Poisson's ratio, μ, the value for the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer can be explicitly determined. The value for the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer, based on the right-hand side of Equation 1F, can be calculated using measured glass properties.
The calculated value for the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer based on measured glass properties is also equivalent to the maximum value for the term {Qheater/Aheater}*{tdielectric/kdielectric} as seen in Equation 1B. The maximum allowed value of the term {Qheater/Aheater}*{tdielectric/kdielectric} explicitly determines the maximum allowed value for the thickness, tdielectric based on the maximum applied heat flux, Qheater/Aheater through the glass thick-film printed and fired first electrically insulative layer during heat-up of the first plate and the thermal conductivity, kdielectric of the glass thick-film printed and fired first electrically insulative layer.
The thickness of the first plate of high thermal conductivity material of the isothermal cooking plate assembly is optimized to [a] provide the thermal conductance required to maintain a substantially uniform temperature across the entire surface of the first plate in the presence of varying heat dissipation rates across the entire surface of the first plate while [b] minimizing the time required to heat up the first plate of the isothermal cooking plate assembly to the user-selected set-point temperature. The thermal conductance between the electrically resistive heating element and the first plate is selected to be sufficiently high to enable the first plate to be heated to the selected set-point temperature within several tens of seconds. By way of example, the first plate of the present disclosure can be heated from room temperature to 150 C within less than 30 seconds for resistive heating elements energized with a maximum applied alternating current of 20 amps at an applied line voltage of 115 volts.
The operating temperature of the first plate of the isothermal cooking plate assembly of the present disclosure may be fixed or may be operator selectable and controlled with a temperature feedback control system design. The temperature feedback control system design utilizes a temperature sensor (e.g., thermocouple) that is in thermal communication with the first plate to regulate the application of power to a heater circuit assembly to maintain the first plate at the operator selected set-point (i.e., cooking) temperature. This controller design incorporating a temperature sensor is referred to hereinafter as temperature feedback control.
A thick-film printing process is used to first print one or more glass or glass-based first electrically insulative layers on the first surface of the first plate. The maximum level of heat flux, {Qheater/Aheater} transferred through the glass thick-film printed and fired first electrically insulative layer corresponds to the heat flux level that occurs during the initial rapid heat-up of the first plate to the operator selected set point temperature (e.g., 150 C). The maximum allowed value for the thickness, tdielectric of the glass thick-film printed and fired first electrically insulative layer represents the maximum allowable thickness of the first electrically insulative layer that avoids the fracture, cracking and/or breaking of the thick-film printed and fired first electrically insulative layer during rapid heat-up of the aluminum first plate. The maximum allowed value for the thickness, tdielectric of the glass thick-film printed and fired first electrically insulative layer can be calculated by rearranging the terms in Equation 1F as seen below in Equation 1G:
{Qheater/Aheater}*{tdielectric/kdielectric}={σdielectric*(1−μ)}/{αdielectric*Edielectric}tdielectric={σdielectric*(1−μ)}/{αdielectric*Edielectric}*{kdielectric/(Qheater/Aheater)} Equation 1G
As seen in Equation 1G, maximum allowed value for the thickness, tdielectric of the glass thick-film printed and fired first electrically insulative layer can be calculated based on the known maximum level of applied heat flux, {Qheater/Aheater} and thermal conductivity, kdielectric of the glass thick-film printed and fired first electrically insulative layer as well as the known properties of glass including the breaking strength of glass, σdielectric, modulus of elasticity, Edielectric, coefficient of thermal expansion, αdielectric and Poisson's ratio, μ.
The incorporation a first plate of high thermal conductivity material (e.g., Aluminum Type 1100) provides heat conduction throughout the extent of the plane of the first plate so that regions of higher heat dissipation in contact with food and required for cooking receive thermal power [a] by heat conduction across the thickness of the first plate from the electrically resistive heating element positioned directly opposite the region of higher heat dissipation and [b] by lateral heat conduction within in the plane of the first plate of high thermal conductivity material from the electrically resistive heating elements located in the regions surrounding the region of higher heat dissipation.
The side of the first plate of high thermal conductivity material opposite the top cooking surface and containing the thick-film printed and fired heater circuit assembly may be thermally insulated to reduce unwanted heat loss from the side of the first plate that is opposite the top cooking surface. By way of example, a rigid second plate of low thermal conductivity material covers the entire surface of the first plate of high thermal conductivity material on the side opposite the top cooking surface. The second plate of low thermal conductivity material (i.e., thermally insulative material) may be selected from the family of plastic materials including, for example, polyphenylene sulfide, polyamide-imide, polyetherimide, and polyetheretherkeytone offering low thermal conductivity, durability, and capability to withstand continuous operation at temperatures of 200 C or greater. An air gap is introduced between the back side of the thermally conductive first plate on which the heater circuit assembly is disposed and the front side of the thermally insulative second plate in order to reduce heat losses from the back side of the first plate. By way of example, the thermally insulative second plate may be attached to the first plate using an intervening high-temperature gasket material around the perimeter (e.g., silicone gasket) to effect a small air gap (e.g., 0.1 to 0.2 inch) between the plates, thereby providing high thermal impedance and low heat loss from the heater side of the first plate due to the very low thermal conductivity of air. Alternatively, the front side of the thermally insulative second plate may be positioned opposite the back side of the thermally conductive first plate on which the heater circuit assembly is disposed with an air gap while not mechanically attached to the first plate.
Further disclosed is an example method for manufacturing an isothermal cooking plate assembly having first plate, thick-film printed and fired heater circuit assembly and second plate that functions as both a thermal insulation covering over the back side (i.e., side opposite the cooking surface of first plate) of first plate as well as a support for first plate. The method of manufacture includes the steps:
The disclosure, accordingly, comprises the apparatus, method, and system possessing the construction, combination of elements, arrangement of parts and steps, which are exemplified in the following detailed description.
For a fuller understanding of the nature and advantages of the present method and process, reference should be made to the following detailed description taken in connection with the accompanying drawings, in which:
The drawings will be described in greater detail below.
In the disclosure to follow, initially described is an isothermal cooking plate assembly incorporating a thermally conductive aluminum first plate having a uniform thickness, which is covered by and in good thermal communication with a durable non-stick coating on the cooking-surface side. The thermally conductive cooking plate is heated by thick-film printed and fired electrically resistive circuit elements combined with thick-film printed and fired electrically conductive leads, both disposed upon a first electrically insulative layer. An optional electrically insulative layer may be disposed over the electrically resistive circuit elements and electrically conductive leads. The first electrically insulative layer, after firing, comprising one or more thick-film printed and fired electrically insulative layers, is selected to be sufficiently small and the associated temperature gradient through the first electrically insulative layer is sufficiently small during the application of the maximum power level and heat flux during rapid heat-up to prevent fracture, cracking and/or breaking of the first electrically insulative layer due during the rapid heat-up of first plate to set-point temperatures of at least 150 C.
Heat transfer analyses and heat-up rate analyses are performed on alternative first plate designs to determine the range of first plate dimensions that achieve the primary objectives of [a] an isothermal cooking plate assembly in which the temperature of the one or more regions or zones of the first plate in contact with the food being cooked remain substantially equivalent to the operator-selected set-point temperature (e.g., 150 C) and [b] an isothermal cooking plate assembly in which the first plate heats up from room temperature (e.g., 25 C) to the operator-selected set-point temperature (e.g., 150 C) within a brief period of time (e.g., a period not exceeding 30 seconds). For the sake of clarity, it should be emphasized that computer program based heat transfer analyses confirm that regions of the first plate not in contact with food can rise more than 10 C above the set-point temperature, since they are only in contact with air. However, their operation beyond “isothermal” conditions specified herein (i.e., within 10 C of the set-point temperature) are of no consequence since only regions of the first plate in contact with food affect the intended cooking of the food whose rate depends on the temperature of the first plate subregions in contact with the one or more articles of food.
Returning to Equation 1F, the term {Qheater/Aheater}*{tdielectric/kdielectric} refers to the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer” that can be induced in the glass thick-film printed and fired first electrically insulative layer without inducing fracture, cracking and/or breaking of the first electrically insulative layer and associated failure of the thick-film printed and fired heater circuit assembly. As seen in Equation 1F, for a given maximum heat flux, Qheater/Aheater through the glass thick-film printed and fired first electrically insulative layer, the value of the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer, as specified by the term {Qheater/Aheater}*{tdielectric/kdielectric} can be determined by calculating the maximum allowable temperature difference {T1−T2}max between the first surface and second surface of the first electrically insulative layer. The maximum allowable temperature difference {T1−T2}max is calculable using equation 1E and given by the term {σdielectric*(1−μ)}/{αdielectric*Edielectric}.
Values for the breaking strength of glass, σdielectric (in units of pounds/square inch or psi) have been measured by Preston as a function of the duration of the stress, sd (in units of microseconds) using the equation:
σdielectric=65,000/{log10(sd/6)} (Equation 1H)
In this regard, see Preston, F. W., The Mechanical Properties of Glass. Journal of Applied Physics 1942; 13: 623-634 and Preston, F. W., Strength of Glass and Duration of Stressing. Nature 1945; 3950:55. For the case of the application of the maximum heat flux through the first electrically insulative layer during a 30 second heat-up period (i.e., maximum stress duration period of 30 seconds), the calculated breaking stress of glass, σdielectric is 9,700 psi. Another reported practical value for the breaking strength of glass, σdielectric is 10,000 psi as reported by R. Lehman (see Lehman, R., The Mechanical Properties of Glass. Glass Engineering Course 150:312 at Rutgers State University of New Jersey 2000). Yet another practical value for the breaking strength of glass, σdielectric is 11,000 psi at atmospheric pressure for a 30 second stress duration period during heat-up of 30 seconds during which the maximum heat flux is applied through the first electrically insulative layer (see Shand, E., Experimental Study of Fracture of Glass: I, The Fracture Process, Journal of American Ceramic Society 1954; 37 (12); 559-572). Based on published values, the nominal breaking strength of glass, σdielectric is about 10,000 psi. The term “practical breaking strength” is used to distinguish the glass breaking strengths in actual applications from the theoretical breaking strength of glass that is based on the stress required to break chemical bonds in glass. The practical breaking strength of glass is orders of magnitude lower than the theoretical breaking strength due to the unavoidable presence of defects and flaws within actual glass layers.
The maximum allowable temperature difference {T1−T2}max specified in Equation 1E also includes other terms including the coefficient of thermal expansion, αdielectric, modulus of elasticity, Edielectric and Poisson's ratio, μ. In the present invention, the coefficient of expansion, αdielectric is required to closely match the coefficient of thermal expansion of aluminum (viz., 21×10−6 per degree C.). In this regard, glasses are reported having coefficients of thermal expansion ranging from 16 to 21×10−6 per degree C. that are intended for bonding to aluminum. In this regard, see U.S. Pat. No. 5,262,364 and Wilder, J. A., Glass Ceramics for Sealing to High Expansion Metals. Sandia National Laboratories 1980; Report No. SAND80-2192:1-26.
Values for the modulus of elasticity, Edielectric (also known as Young's modulus) for glasses have also been reported to be in the range 9.2×106 psi to 10.3×106 psi. In this regard, see Matsuda, J., Studies on the Young's Modulus of Silicate Glass as a Function of Temperature. Review of Physical Chemistry of Japan 1960; 30 (1):9-24 and Preston. F. W., The Mechanical Properties of Glass. Journal of Applied Physics 1942; 13: 623-634. In addition, the modulus of elasticity, Edielectric for glasses having a large coefficient of thermal expansion is reported to range from 10.2×106 to 10.3×106 psi. In this regard, see Thermal Loads on Optical Glass. Schott Technical Information-Advanced Optics October 2018; TIE-32: 1-6.
The value for Poisson's ratio for glasses having a large coefficient of thermal expansion (e.g., 13×10−6 to 14×10−6 per degree Centigrade) is reported to be 0.30 (see Thermal Loads on Optical Glass. Schott Technical Information-Advanced Optics October 2018; TIE-32: 1-6). Also, the value for Poisson's ratio for glass has been reported to be 0.25 (see Preston. F. W., The Mechanical Properties of Glass. Journal of Applied Physics 1942; 13: 623-634). In addition, Poisson's ratios for 12 different glasses are reported to range from 0.26 to 0.30 (see Kannappan, A., et. al., Elastic and Mechanical properties of Glass Specimen by Ultrasonic Method. Asian Research Publishing Network Journal of Engineering and Applied Sciences 2009; 4(1): 27-31).
The nominal properties values for glass including the [a] breaking strength of glass, σdielectric, [b] modulus of elasticity, Edielectric of glass, [c] coefficient of thermal expansion, αdielectric of glass that matches the coefficient of thermal expansion of aluminum and [d] Poisson's ratio, μ for glass can be combined in Equation 1E to calculate the maximum allowable temperature difference {T1−T2}max. The maximum allowable temperature difference {T1−T2}max corresponds to the temperature of the first surface, T1′ and the temperature of the second surface, T2′ of the first electrically insulative layer. The value for the Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer, {T1−T2}max is calculated, as follows:
(T′1−T′2)max={σdielectric*(1−μ)}/{αdielectric*Edielectric}
(T′1−T′2)max={10,000psi*(1−0.30)}/{21×10−6/C*9.7×106psi}
(T′1−T′2)max=34.4C
Returning to Equation 1B, this equation can be rearranged so the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer can be expressed in terms of Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer, {T1−T2}max, the heat flux, Qheater/Aheater and the thermal conductivity, kdielectric of the thick-film printed and fired first electrically insulative layer as seen in Equation 1I:
(T1′−T2′)={Qheater/Aheater}*{tdielectric/kdielectric}
tdielectric={(T1′−T2′)*kdielectric}/{Qheater/Aheater} (Equation 1I)
The calculated Maximum Allowable Thermal Gradient in the First Electrically Insulative Layer, {T1−T2}max can next be substituted into the above Equation 1I for the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer as seen in Equation 1J:
tdielectric={34.4*kdielectric}/{Qheater/Aheater} (Equation 1J)
In this first example, as seen in Equation 1J, the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer is determined based on the thermal conductivity, kdielectric of the thick-film printed and fired first electrically insulative layer and the maximum applied heat flux, {Qheater/Aheater} during the rapid heat-up of the first plate. By way of this first example, the overall dimensions of a first plate of an isothermal cooking plate assembly of a griddle system are 6.0 inches×9.0 inches. The total area of 19 thick-film printed and fired second electrically resistive heating element legs (as seen in
Continuing with this first example, a first preferred commercially available material for the thick-film printed and fired first electrically insulative layer is the AS100 dielectric paste manufactured by DuPont Microcircuit Materials, Research Triangle Park, North Carolina. This dielectric paste, developed for thick-film printing and firing on aluminum substrates, has a coefficient of thermal expansion, αdielectric that closely matches the coefficient of thermal expansion of aluminum (viz., 21×10−6 per degree C.). The measured thermal conductivity of the thick-film and fired AS100 dielectric material is 0.0016 watts/cm-C, as reported in the DuPont AS100 Technical Data Sheet issued by DuPont Microelectronic Materials in August 2014. The above Equation 1I for the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer, as specified above in Equation 1J, can be expressed as follows:
tdielectric={34.4*kdielectric}/{Qheater/Aheater}
tdielectric={34.4*0.0016 watts/cm-C}/7.43 watts/sq·cm.
tdielectric=0.0074 cm=0.0029 inch
Based on the above first example, a thick-film printed and fired first electrically insulative layer having a coefficient of thermal expansion, αdielectric substantially the same as the aluminum first plate and nominal values for glass (viz., breaking strength, σdielectric equal to 10,000 psi, modulus of elasticity, Edielectric equal to 9.2×106 psi and Poisson's ratio, μ equal to 0.3), a thermal conductivity of 0.0016 watts/cm-C and a maximum heat flux of 7.43 watts/sq·cm., the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer should not exceed 0.0029 inch in order to avoid fracture, cracking and/or breaking of the first thermally insulative layer.
However, to avoid “pin-holes” in the electrically insulative layer (i.e., very small defects due to incomplete coverage of the substrate by the thick-film and fired electrically insulative layer), the manufacturer of this thick-film dielectric paste specifies thick-film printing and firing a first layer of the thick-film printed electrically insulative layer followed by a second thick-film printing and firing of the electrically insulative layer resulting in a total thickness of 0.0014 inch (35 microns). In this regard, see DuPont AS100 Technical Data Sheet issued by DuPont Microcircuit Materials in August 2014. This two stage thick-film printing and firing process eliminates the possibility of “pin hole” defects in the overall first electrically insulative layer, thereby eliminating unwanted electrical current flow paths through the first electrically insulative layer. In this first example, the total thickness of the thick-film printed and fired electrically insulative layer having two layers (viz., 0.0014 inch) is substantially less than the maximum allowable thickness, tdielectric for this example thick-film printed and fired heater circuit assembly (viz., 0.0029 inch), thereby avoiding the possibility of fracture, cracking and/or breaking of the first thermally insulative layer.
In this second example, as seen in Equation 1J, the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer is determined by the thermal conductivity, kdielectric of the thick-film printed and fired first electrically insulative layer and the maximum applied heat flux, {Qheater/Aheater}. By way of this second example, the overall dimensions of a first plate of an isothermal cooking plate assembly of a griddle system are 6.0 inches×9.0 inches. The total area of 19 thick-film printed and fired second electrically resistive heating element legs (as seen in
Continuing with this second example, a second preferred commercially available material for the thick-film printed and fired first electrically insulative layer is the IP6075 dielectric paste manufactured by Heraeus Electronics, Heraeus Deutschland GmbH & Co. KG, Hanau, Germany. This dielectric paste, developed for thick-film printing and firing on aluminum substrates, has a coefficient of thermal expansion, αdielectric that closely matches the coefficient of thermal expansion of aluminum (viz., 21×10−6 per degree C.). The measured thermal conductivity of the thick-film and fired IP6075 dielectric material is 0.0010 watts/cm-C, as reported in the Celcion IP6075 Technical Data Sheet issued by Heraeus Electronics in 2016. The above Equation 1I for the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer, as seen in Equation 1J, can be expressed as follows:
tdielectric={34.4*kdielectric}/{Qheater/Aheater}
tdielectric={34.4*0.0010 watts/cm-C}/7.43 watts/sq·cm.
tdielectric=0.0046 cm=0.0018 inch
Based on the above second example, a thick-film printed and fired first electrically insulative layer having a coefficient of thermal expansion, αdielectric substantially the same as the aluminum first plate and nominal values for glass (viz., breaking strength, σdielectric equal to 10,000 psi, modulus of elasticity, Edielectric equal to 9.2×106 psi and Poisson's ratio, μ equal to 0.3), a thermal conductivity of 0.0010 watts/cm-C and a maximum heat flux of 7.43 watts/sq·cm., the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer must not exceed 0.0018 inch in order to avoid fracture, cracking and/or breaking of the first thermally insulative layer.
However, to avoid “pin-holes” in the electrically insulative layer (i.e., very small defects due to incomplete coverage of the substrate by the thick-film and fired electrically insulative layer), it is common to thick-film print and fire a first layer of the thick-film printed electrically insulative layer followed by a second and optionally a third thick-film printed and fired electrically insulative layer to eliminate the possibility of “pin hole” defects in the overall first electrically insulative layer, thereby eliminating unwanted electrical current flow paths through the first electrically insulative layer.
The minimum thickness of each thick-film printed and fired electrically insulative layer is specified by the thick-film paste manufacturer to be 0.0008 inch (20 microns). Consequently, the requirement to thick film print and fire a second layer of the electrically insulative layer will result in a total thickness of the first electrically insulative layer, tdielectric following the second thick film printing and firing of an electrically insulative layer of 0.0016 inch. In this regard, see Celcion IP6075 Technical Data Sheet issued by Heraeus Electronics in 2016. This total thickness of the first electrically insulative layer, tdielectric comprising two thick-film printed and fired layers is less than maximum allowable thickness, tdielectric for this example thick-film printed and fired heater circuit assembly (viz., 0.0018 inch). However, the printing of a third thick-film printed and fired electrically insulative layer will result in a total fired thickness of 0.0024 inch, as recommended by the manufacturer in the Celcion IP6075 Technical Data Sheet issued by Heraeus Electronics in 2016. If a third layer of the Celcion IP6075 dielectric paste is printed and fired, then the total thickness for all three printed and fired layers (viz., 0.0024 inch) would exceed the maximum allowable thickness, tdielectric for this example thick-film printed and fired heater circuit assembly (viz., 0.0018 inch) by 33%, thereby resulting in the likelihood of the fracture, cracking and/or breaking of this first electrically insulative layer comprising three separately thick-film printed and fired electrically insulative layers.
In this third example, as seen in Equation 1J, the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer is determined by the thermal conductivity, kdielectric of the thick-film printed and fired first electrically insulative layer and the maximum applied heat flux, {Qheater/Aheater}. By way of this third example, the overall dimensions of a first plate of an isothermal cooking plate assembly of a griddle system are 5.0 inches×6.0 inches. The total area of 19 thick-film printed and fired second electrically resistive heating element legs (as seen in
Continuing with this third example, a second preferred commercially available material for the thick-film printed and fired first electrically insulative layer is the IP6075 dielectric paste manufactured by Heraeus Electronics, Heraeus Deutschland GmbH & Co. KG, Hanau, Germany. This dielectric paste, developed for thick-film printing and firing on aluminum substrates, has a coefficient of thermal expansion, αdielectric that closely matches the coefficient of thermal expansion of aluminum (viz., 21×10−6 per degree C.). The measured thermal conductivity of the thick-film and fired IP6075 dielectric material is 0.0010 watts/cm-C, as reported in the Celcion IP6075 Technical Data Sheet issued 2016. The above Equation 1I for the maximum allowed thickness, tdielectric of the thick-film printed and fired first electrically insulative layer, as seen above in Equation 1J, can be expressed as follows:
tdielectric={34.4*kdielectric}/{Qheater/Aheater}
tdielectric={34.4*0.0010 watts/cm-C}/14.86 watts/sq·cm.
tdielectric=0.0023 cm=0.0009 inch
Based on the this third example, a thick-film printed and fired first electrically insulative layer having a coefficient of thermal expansion, αdielectric substantially the same as the aluminum first plate and nominal values for glass (viz., breaking strength, σdielectric equal to 10,000 psi, modulus of elasticity, Edielectric equal to 9.2×106 psi and Poisson's ratio, μ equal to 0.3), a thermal conductivity of 0.0010 watts/cm-C and a maximum heat flux of 14.86 watts/sq·cm., the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer must not exceed 0.0009 inch in order to avoid fracture, cracking and/or breaking of the first electrically insulative layer.
However, to avoid “pin-holes” in the electrically insulative layer (i.e., very small defects due to incomplete coverage of the substrate by the thick-film and fired electrically insulative layer, it is common to thick-film print and fire a first layer of the thick-film printed electrically insulative layer followed by a second and even a third thick-film printed and fired to eliminate the possibility of “pin hole” defects in the overall first electrically insulative layer, thereby eliminating unwanted electrical current flow paths through the first electrically insulative layer.
Since the minimum of thickness of each thick-film printed and fired electrically insulative layer is specified by the thick-film paste manufacturer to be 0.0008 inch (20 microns), then the requirement to thick film print and fire a second layer of the electrically insulative layer will result in a total thickness of the first electrically insulative layer, tdielectric following the second thick film printing and firing of up to 0.0016. This total thickness of the first electrically insulative layer, tdielectric exceeds the maximum allowable thickness, tdielectric for this example thick-film printed and fired heater circuit assembly (viz., 0.0009 inch) by 77% and the likelihood of the fracture, cracking and/or breaking of the first electrically insulative layer.
As seen in Equation 1J and specified above in Examples 1, 2 and 3, the maximum allowed thickness, tdielectric of a thick-film printed and fired first electrically insulative layer is directly proportional to the thermal conductivity, kdielectric of the first electrically insulative layer (following printing and firing) and is inversely proportional to the maximum applied heat flux. The maximum applied heat flux occurs during the rapid heat-up of the first plate of an isothermal cooking plate assembly of a griddle system. As seen in Examples 2 and 3 above, the requirement for thick-film printing and firing of two to three separate layers of the thick-film printed and fired electrically insulative layer can exceed the maximum allowable thickness, tdielectric depending on the thermal conductivity, kdielectric and the maximum applied heat flux, {Qheater/Aheater} of the thick-film printed and fired first electrically insulative layer.
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First plate 52 of high thermal conductivity material may be machined from Type 1100 aluminum plate or Type 6061 aluminum plate, both available from McMaster-Carr Supply Company (Cleveland, Ohio). Second plate 30 of low thermal conductivity material may be injection molded from a plastic material with a high service temperature of at least 150 C. By way of example, second plate 30 of low thermal conductivity material may be injection molded from [a] RYTON® polyphenylene sulfide resin available from Chevron-Phillips Chemical Company (Woodlands, Texas) or [b] ULTEM® 1000 polyetherimide resin available from Sabic Corporation (Pittsfield, Massachusetts). By way of example, thermally insulative mounting support member 110 may be machined from DELRIN© (registered trademark of E.I. du Pont de Nemours and Company, Wilmington, Delaware) acetal resin bar stock available from McMaster-Carr Supply Company (Cleveland, Ohio).
The uniformly thick first plate 52 of high thermal conductivity material may optionally be roll bonded on the top cooking surface 28 with a cladding layer (not shown in figures), for instance, formed of austenitic stainless steel, such as a Type 304. The preferred thickness of the cladding layer is in the range 0.002 to 0.010 inch, more preferably 0.002 inch to 0.004 inch. A small cladding thickness is preferred to minimize the effect of the added volume of cladding material on the time to heat up the first plate 52 of isothermal cooking plate assembly 50 from room temperature to the operator-selected set-point temperature.
In a preferred embodiment seen in
First plate 52, thick-film printed and fired heater circuit assembly 130 and second plate 30 combine to form cooking plate assembly 50 that is mechanically attached to the griddle system and replaceable in the field by mechanically disconnecting the first and second electrical leads 158 and 160 from first and second contact pads 62 and 64, respectively, and by mechanically disconnecting temperature sensor 39 from the first plate and mechanically disconnecting cooking plate assembly from the griddle system. The arrangement of mechanical fastening attachments seen in
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Isothermal Cooking Plate Heat Transfer Analyses
The preferred design of the first plate 52 of the isothermal cooking plate assembly 50 of the present disclosure is capable of rapid heat-up from 25 C (i.e., room temperature) to a cooking temperature of 150 C within less than about 30 seconds using up to 20 amps at 115 to 120 volts (i.e., widely available line power) while maintaining the cooking surface 28 of first plate 52 within 10 degrees C. of the set-point temperature (e.g., 150 C) throughout the entire zone of food 53 being cooked at loading factors up to 60% (as defined below). The attainment of a rapid heat-up, isothermal cooking plate assembly 50 for a full range of cooking conditions using widely available 115-volt line power required the optimization of the first plate 52 surface area, length-to-width aspect ratio of first plate 52, thickness, t2 of first plate 52 and material of construction of first plate 52. The optimization of the design of the isothermal cooking plate assembly 50 of the present disclosure was achieved by performing heat transfer analyses for a full range of first plate 52 lengths, widths, thicknesses, materials of construction and loading factors. The term “loading factors” refers to the amount of food 53 simultaneously being cooked and the distribution of portions of food 53a, 53b, on the cooking surface 28 of first plate 52. The unit of measure of loading factor is a percentage and refers to the fraction of the total cooking surface 28 of first plate 52 covered by one or more portions of food 53. For example, if the combined area of the articles of food 53 being cooked is 20 in2 and the cooking surface 28 area of first plate is 50 in2, then the loading factor is 20/50 in2 or 40%.
The thermal model used in these heat transfer analyses accurately represents actual known cooking conditions for commercially available griddles. In this regard, the cooking industry has developed uniform testing procedures to evaluate the performance and efficiency of commercially available cooking appliances (see Kaufman, D., et. al., “Development of Uniform Testing Procedures for Commercial Cooking Appliances-Griddles”, Archives of American Council for Energy Efficient Economy, 1988 Archives, ACEEE 1988 Proceedings, Volume 4-008, pages 4.70-4.81).
The test procedure described in the above referenced report includes the specification of the standard food portion used to evaluate the performance and efficiency of griddles. The standard food portion is one or more one-quarter pound hamburger patties containing 20% fat (by weight) and moisture content of 60% to 65%. The amount of energy transferred to the hamburger food portion in the above referenced study was determined to be 475 BTU/pound of hamburger. In the cited standard testing procedure, the adequate cooking of the standard hamburger patty was achieved in 7.83 minutes or 0.1305 hours. The above standardized energy requirement of 475 BTU/pound of hamburger delivered in 0.1305 hours results in a heating power input of 3,640 BTU/hour per pound of hamburger, which is equivalent to 1,067 watts per pound of hamburger or 267 watts per one-quarter pound hamburger. The thermal model assumed each food portion was a one-quarter pound hamburger and the average heat input, Qfood during the period of cooking each one-quarter pound hamburger was 267 watts. The heat input per unit area or heat flux into the portion of food 53 was determined by dividing 267 watts by the area of the portion of food 53 (e.g., hamburger patty). The example thermal model seen in
Those portions of the cooking surface 28 of the first plate 52 not covered by one or more portions of food 53 were assumed to dissipate heat 332 to the environment by free convection heat transfer and radiation heat transfer based on a surface emittance of 0.9 corresponding to the actual radiation emittance of typical non-stick coatings. The free convection heat transfer, Qconv from each of the exposed cooking surfaces of each first plate subregion 304 of first plate 52 that are not covered by one or more portions of food 53. The free convection heat transfer, Qconv is based on the well-known convection heat transfer equation:
Qconv=h*Asubregion*(Tsubregion−T0) (Equation 1I)
In the above Equation 1I, the free-convection heat transfer coefficient, h for a horizontal plate facing upward is 9.5×104 watts/(cm2-C). The term Asubregion in the above equation refers to the exposed surface area (in units of square centimeters) of each of the first plate subregions 304 not covered by a food portion subregion 306 of food portion 53. The term Tsubregion refers to the temperature of each first plate subregion 304 and the term T0 refers to the ambient or room temperature, both in same units of either degrees Celsius (C) or degrees Kelvin (K).
The radiation heat transfer, Qrad from each of the exposed cooking surfaces of each first plate subregion 304 the of the first plate 52 that are not covered by one or more portions of food 53 is based on the well-known radiation heat transfer equation:
Qrad=σ*ε*Asubregion*(T′subregion4-T′04) (Equation 2)
In the above Equation 2, σ refers to the Stefan-Boltzmann constant that has the value 5.67×10−12 watts/cm2-K4. The term ε refers to the radiation emittance of the exposed surface of each of the first plate subregions 304 not covered by a food portion subregion 306 of food portion 53. For the assumed covering of the cooking surface 28 of first plate 52 with a non-stick coating, the corresponding unitless radiation emittance of such coatings is nominally 0.9. The term Asubregion in the above equation refers to the exposed surface area (in units of square centimeters) of each of the first plate subregions 304 not covered by a food portion subregion 306 of food portion 53. The term T′subregion refers to the temperature of each first plate subregion 304 and the term T′0 refers to the ambient or room temperature, both in the same units of degrees Kelvin (K) since the Stefan-Boltzmann constant is in reciprocal units of degrees Kelvin raised to the fourth power. The absolute Kelvin temperature scale is defined as the temperature in degrees Centigrade plus 273. By way of example, a temperature of 150 Centigrade corresponds to a temperature of 150 C+273 or 423 Kelvin.
The thermal model used for the heat transfer analysis of alternative designs for a first plate 52 is based on distributed uniform heating by a heater circuit assembly 130 surmounted on essentially the entire back surface area 159 of first plate 52 as seen in
At the geometrical center of each first plate subregion 304 is a temperature node 308 corresponding to the computed temperature for each the first plate subregion 304. Each heat transfer analysis case produced a total of 320 temperatures at each temperature node 308 corresponding to each of the 320 first plate subregions 304.
The heat input per unit area of the portion of food 53 discussed above (viz., 267 watts per one-quarter pound hamburger divided by the area of the portion of food 53) was converted into the heat input for each food portion subregion 306 supplied by each corresponding adjacent first plate subregion 304 in direct contact with the adjacent food portion subregion 306 as seen in
The total heat input, Qtotal that is required to be generated within the heater circuit assembly 130 surmounted on each first plate 52 of the isothermal cooking plate assembly 50 is initially estimated by combining the total heat required for cooking one or more food portions 53, Qfood with the estimated free convection heat dissipation, Qconv and estimated radiation heat dissipation, Qrad from the exposed surfaces of first plate 52 not covered by one or more food portions 53. An energy balance equation is solved by iterative heat transfer analyses using an incrementally adjusted value for the total heat input, Qtotal until the first plate subregion 304 at the corresponding thermocouple location 43 is at the specified set-point temperature (e.g., 150.0 C) as seen in
The heat transfer analyses were performed using a thermal analysis computer program developed and validated by the Lawrence Livermore Laboratory and known as the TRUMP computer program (see Edwards, Arthur L., “TRUMP: A Computer Program for Transient and Steady-State Temperature Distribution in Multidimensional Systems”, UCRL-14754, Rev. 3, Lawrence Livermore Laboratories, 1972), the disclosure of which is expressly incorporated herein by reference. There are at least a dozen other heat transfer computer programs that could alternatively be used for the thermal analyses performed for the present disclosure including [1] ANSYS Computer Program available from ANSYS, Inc., Canonsburg, Pennsylvania and [2] NASTRAN Computer Program available from MSC Software, Newport Beach, California. The TRUMP thermal analysis computer program, like other similar thermal analysis computer programs, solves general nonlinear parabolic partial differential equations describing flow in various kinds of potential fields such as temperature fields.
The steady state heat transfer analysis performed by the TRUMP computer program involves a first plate 52 comprising a continuous sheet of high thermal conductivity material having a uniform thickness, t2. The flow of a quantity of heat, q, within the first plate 52 is via conduction heat transfer governed by the well-known conduction heat transfer provided below:
q=kaluminum*(Acond/Lcond)*(T2−T1) (Equation 3)
The heat flow, q in Equation 1 is in units of watts. The term kaluminum in Equation 1 refers to the thermal conductivity of the material comprising first plate 52 and is expressed in units of watts/cm-C. The term Acond in Equation 3 represents the cross-sectional area through which heat flows from a first region to a second region. In the thermal model illustrated in
By way of example and referring to
q(304a,304b)=kaluminum*((W29*t2)/L14)*(T304b−T304a) (Equation 4)
For the case of an Aluminum 1100 first plate 52 having a thermal conductivity of 2.18 watts/cm-C, a thickness t2 of first plate 52 of 0.635 cm, a length L14 of 1.00 cm and width W29 of 1.00 cm, Equation 4 can be expressed as follows:
q(304a,304b)=2.18*0.635*(T304b−T304a) (Equation 5)
As seen in Equation 4, the larger the value of the thermal conductivity, kaluminum of first plate 52 and the larger the value of thickness, t2 of first plate 52, the larger the amount of heat that can be conducted between adjacent first plate subregions 304 for a given temperature difference or gradient (T304b−T304a). Therefore, since one of the objectives of the present disclosure for an isothermal cooking plate assembly 50 is to enable the largest amount of heat to be conducted under conditions of small temperature differences between the set-point temperature and temperatures within the region of the portion of food 53 being cooked, the thermal conductivity of the first plate 52 should be large and the thickness, t2 of the first plate 52 should be large.
The term “isothermal” as used herein refers to the achievement of temperatures within the region(s) of the portion(s) of food 53 being cooked that are substantially the same or within not greater than 10 C of the set-point temperature of the isothermal cooking plate assembly 50. For set-point temperatures up to 230 C (450 F), the criterion for achieving an isothermal cooking plate assembly 50 is the requirement that the temperatures within the region(s) of the portion(s) of food 53 being cooked are within about 10 C of the set-point temperature.
However, it is also one of the objectives of the present disclosure to provide an isothermal cooking plate assembly 50 that can be heated from room temperature to a user selected set-point temperature (e.g., 150 C) within a brief period of less than 30 seconds to maximize the energy and operator time efficiency associated with cooking food. The capability to heat first plate 52 of an isothermal cooking plate assembly 50 from room temperature to 150 C within 30 seconds or less enables the consumption of electrical power and expenditure for associated electricity costs only when a requirement for cooking food occurs (e.g., a customer orders one or more cooked hamburgers or other cooked food items).
The time required for the heat-up of an isothermal cooking plate assembly 50 from room temperature to a user selected set-point temperature for the first plate 52 of the isothermal cooking plate assembly 50 is determined by the well known equation for heat capacitance of a known volume of material having defined values of density and specific heat. By way of example, the time required to heat a first plate 52 plate from 25 C to 150 C having known dimensions and constructed using a known material is based on the well known definition of the specific heat, C of any material. The specific heat of any material is the amount of heat, Q required to raise the temperature, T of the mass, m of one gram of material by one degree Celsius. Based on the definition of the specific heat of a material, the rate of heat up, ΔT/Δt at which the temperature, T of a material will increase per unit time, t is given by the well-known equation:
ΔQ/Δt=m*C*ΔT/Δt (Equation 6)
The mass, m, of the first plate 52 of an isothermal cooking plate assembly 50 (in grams) is the product of the volume of the cooking plate, V and the density, ρ of the material comprising the first plate 52 (e.g., Aluminum 1100). Hence, Equation 6 can be expressed in terms of the density, ρ of the material comprising first plate 52 (in units of grams/cm3) and the volume, V of first plate 52 (in units of cm3). Referring to
ΔT/Δt=(ΔQ/Δt)/(L13*W26*t2*ρ*C) (Equation 7)
The calculated time, theatup required to heat up first plate 52 of the isothermal cooking plate assembly 50 to a desired set-point temperature, Tsetpoint is determined by dividing the required temperature rise from room temperature, T0 (e.g., from 25 C) to 150 C or a temperature rise of 125 C by the calculated rate of heat up, ΔT/Δt. Accordingly, the heat-up time for first plate 50 is determined by Equation 7 as shown below:
theatup=(Tsetpoint−T0)/(ΔT/Δt)=(Tsetpoint−T0)*(L13*W26*t2*ρ*C)/(ΔQ/Δt) (Eq. 8)
This computational process was used to calculate the time required to heat up the first plate 52 of isothermal cooking plate assembly 50 from 25 C to 150 C for thicknesses, t2 of first plate 52 ranging from 0.120 inch (0.305 cm) to 0.375 inch (0.953 cm) for a maximum level of applied power, (ΔQ/Δt) of 2300 watts or 549.5 calories/second into heater circuit assembly 130 (corresponding to an input voltage of 115 volts at 20 amps). The specific heat, C of Aluminum 1100, the preferred material for the first plate 52, is 0.216 calories/gram-C and the density of Aluminum 1100 is 2.71 gram/cm3. For comparison purposes with a prior art cooking plate comprised of iron, the specific heat, C value of iron is 0.124 calories/gram-C and the density of iron is 7.87 gram/cm3. The length, L13 and width, W26 of the first plate 52 used in the calculation of heat up rates was based on the results of the thermal analysis of a range of sizes of first plate 52 to determine the range of sizes of first plate 52 that achieved the objective of an isothermal cooking plate assembly 50, viz., a first plate 52 in which the maximum temperature difference, ΔTmax between the set-point temperature, Tsetpoint and any temperature in the zone where an article of food is being cooked does not exceed 10 C for set-point temperatures, Tsetpoint up to 230 C (450 F).
A total of 118 heat transfer analyses were performed using the TRUMP computer program and the thermal models shown in
The temperature distribution among the 320 first plate subregions 304 is influenced by the loading factor of food being cooked. The term “loading factor” refers to the amount of food 53 simultaneously being cooked and the distribution of portions of food 53a, 53b, on the cooking surface 28 of first plate 52. The unit of measure of loading factor is a percentage and refers to the fraction of the total cooking surface 28 of first plate 52 covered by one or more portions of food 53. The effect of the loading factor on the temperature distribution of the 320 first plate subregions 304 was included in the 118 heat transfer analyses by specifying and performing heat transfer analyses on three different thermal models as seen in
The TRUMP computer program was used to perform heat transfer analyses corresponding to 118 different designs for first plate 52 comprising different materials (e.g., Aluminum and iron) and a range of lengths, widths and thicknesses and provided steady-state temperature values for the 320 first plate subregions 304 at their temperature nodes 308 (as seen in
Based on the 118 heat transfer analyses performed using the TRUMP heat transfer computer program, the optimum length, L2 for a single first plate 52 heated by a single heater circuit assembly 130 surmounted on substantially the entire surface area on the back side of the first plate 52 (i.e., opposite the food-cooking surface side) to achieve a maximum temperature difference, ΔTmax that does not exceed 10 C for any operator-selectable set-point temperature, Tsetpoint up to 230 C (450 F) is in the range from 7.2 to 9.0 inch. Also, based on these 118 heat transfer analyses, the optimum width, W3 for a single first plate 52 heated by a single heater circuit assembly 130 surmounted on substantially the entire surface area on the back side of the first plate 52 (i.e., opposite the cooking surface side) to achieve a maximum temperature difference, ΔTmax that does not exceed 10 C for any operator-selectable set-point temperature, Tsetpoint up to 230 C (450 F) is in the range from 6.0 to 7.2 inch. These optimum ranges of lengths, L2 and widths, W3 correspond to a maximum length to width aspect ratio of 9.0 inch/6.0 inch or 1.50.
Once the optimum range of lengths, L2 and widths, W3 for the first plate 52 were determined from the initial set of the heat transfer analyses, than a nominal length, L13 and width, W26 was selected for the purpose of computing the maximum temperature difference, ΔTmax between the set-point temperature, Tsetpoint and any temperature in the zone where an article of food is being cooked. In addition, referring to
The results of the heat transfer analyses of alternative designs for first plate 52 determined the range of allowable length and width dimensions for first plate 52 that met the requirements for maintaining the maximum temperature difference between the operator-selected set-point temperature and any subregion 304 of first plate 52 in contact with one or more articles of food 53 to 10 C or less. The allowable length and width dimensions for first plate 52 (viz., a length in the range 7.2 to 9.0 inches and width in the range 6.0 to 7.2 inches), length-to-width aspect ratio of not greater than 1.5 and surface are not greater than 54 square inches in combination with the allowable range of thicknesses of first plate 52 (viz., 0.187 to 0.275 inch) result in a volume of first plate 52 that can be heated up from 25 C to 150 C in less than 30 seconds using widely available line power of 115 volts at a maximum current of 20 amps. As a consequence, the preferred embodiments of the present disclosure eliminate the need for a 220 volt source of power and all of the associated construction complexities and costs of providing and using this higher voltage electrical service. In addition, the two-fold higher heat flux associated with powering the thick-film printed and fired heater circuit assembly 130 at 220 volts and 20 amps (i.e., 4,400 watts of power) is unnecessary to achieve a rapid heat-up within 30 seconds and only adds to the temperature difference across the interface between the thick-film printed and fired heater circuit assembly 130 and first plate 52. The only advantage of using of a source of 220-volt line power is to reduce the heat-up time from room temperature to the operator-selected set-point temperature. However, a maximum heat-up time of 30 seconds for a griddle system 10 powered by the widely available 115 volts and 20 amps eliminates the need for 220-volt line power source since the further reduction in heat-up time does not compensate for the added cost of supplying 220-volt service and operating the griddle system 10 at the voltage levels and the higher costs associated with the adhesives and the their application for use at the higher heat flux levels associated with the application of 4,400 watts of power per isothermal cooking plate assembly 50.
The results of the heat transfer analysis using the TRUMP computer program for thermal models seen in
Curves 402, 404 and 406 in
Still referring
The first plate 52 is substantially uniform in thickness and in the form of a continuous sheet. The term “continuous sheet”, as used herein to specify first plate 52, refers to a thermally conductive first plate 52 having a substantially uniform thickness without any partial or full thickness cutouts or slots other than [a] a small blind (i.e., partial depth) machined hole 45 at the geometrical center on the side of first plate 52 opposite the cooking side for mechanically securing temperature sensor 39 to first plate 52 and [b] small machined holes at the perimeter corners of first plate 52 opposite the cooking side for mechanically securing first plate 52 to second plate 30 using machine screws 82 having a diameter D3.
As seen in
Still referring to
Still referring to
A preferred arrangement for the removable attachment of first electrical lead wire 158 and second electrical lead wire 160 to first electrical contact pad 62 and second electrical contact pad 64, respectively, is seen in
By way of example, first drilled through-hole 57 and second drilled through-hole 58 have diameters, D14 and extend through the full thickness of second plate 30 of low thermal conductivity material. Mechanical fastening screws 154, 156 traverse first washer-type electrical contact 150 and second washer-type electrical contact 152 respectively, as well as holes 66, 68 in first electrical contact pad 62 and second electrical contact pad 64, respectively. Mechanical fastening screws 154, 156 are received in threaded holes 162 and 164, respectively. Belleville disc springs 166, 168 of height H3 and thickness 118, preferably a stack of at least two, are arranged to maximize deflection distance and are selected having an outside diameter and inside diameter matched to outside diameter, D9 of mechanical fastening screws 154, 156 and outside diameter of washer-type electrical contacts 150, 152. By way of example, stainless steel Type 302 Belleville disc springs 166, 168 are available from McMaster-Carr Supply Company Supply (Cleveland, Ohio).
Still referring to
Still referring to
By way of example, a cross section of thick-film printed and fired heater circuit assembly 130 affixed to bottom surface of first plate 52 of high thermal conductivity material is seen in
A more detailed partial view of a cross section of a thick-film printed and fired heater circuit assembly 130 affixed to bottom surface of first plate 52 of high thermal conductivity material is seen in
As specified in the preceding sections, the thermal conduction of heat, Q through a solid having a substantially uniform thickness, t can be expressed by Equation 1. For the specific case of heat conduction through the thick-film printed and fired first electrically insulative layer 141 of the present invention, the resulting temperature difference, (T1′−T2′) across the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer 141 can be expressed in terms of the amount of heat conducted through the through the thick-film printed and fired first electrically insulative layer, Qheater as well as the area through which heat is conducted, Aheater, the thickness, tdielectric of the thick-film printed and fired first electrically insulative layer and the thermal conductivity, kdielectric of the thick-film printed and fired first electrically insulative layer as seen in Equation 1B. The temperature T1′ refers to the temperature on first surface 155 of first electrically insulative layer 141 as seen in
Referring next to
The range of dimensions for the griddle system 10 and its components, as seen in
L1 = 9.0 to 12.0
L9 = 3.6 to 4.2
L2 = 7.2 to 9.0
L10 = 3.4 to 4.0
L3 = 7.5 to 10.0
L11 = 2.6 to 3.2
L4 = 7.0 to 8.3
L12 = 2.0 to 2.6
L5 = 6.0 to 8.5
L13 = 7.9
L6 = 0.75 to 1.5
L14 = 0.394
L7 = 0.32 to 0.82
L15 = 1.8 to 3.6
W1 = 12 to 54
W16 = 0.05 to 0.20
W2 = 6.3
W17 = 0.05 to 0.25
W3 = 6.0 to 7. 7
W18 = 0.02 to 0.25
W4 = 5.9 to 7.6
W19 = 0.40 to 1.00
W5 = 2.0 to 4.0
W20 = 0.003 to 0.100
W6 = 0.05 to 0.25
W21 = 0.003 to 0.100
W7 = 0.02 to 0.08
W22 = 0.02 to 0.25
W8 = 0.003 to 0.100
W23 = 3.15
W9 = 0.20 to 0.35
W24 = 0.4
W10 = 0.01 to 0.03
W25 = 0.8
W11 = 0.02 to 0.08
W26 = 6.3
W12 = 0.05 to 0.25
W27 = 1.57
W13 = 0.05 to 0.25
W28 = 4.72
W14 = 0.01 to 0.04
W29 = 0.394
W15 = 0.30 to 0.80
W30 = 2.9 TO 3.4
H1 = 4.0 TO 10.0
W31 = 2.37
H2 = 2.0 TO 6.0
W32 = 0.79
H3 = 0.012 to 0.030
D8 = 0.11 to 0.22
D2 = 0.10 to 0.20
D9 = 0.10 to 0.20
D3 = 0.10 to 0.20
D10 = 0.110 to 0.220
D4 = 0.10 to 0.20
D11 = 0.120 to 0.250
D5 = 0.10 to 0.20
D12 = 0.120 to 0.250
D6 = 0.10 to 0.25
D13 = 0.110 to 0.220
D7 = 0.187 to 0.375
D14 = 0.187 to 0.375
t1 = 0.02 to 0.10
t10 = 0.02 to 0.08
t2 = 0.150 to 0.250
t11 = 0.0005 to 0.005
t3 = 0.25 to 0.75
t12 = 0.0002 to 0.0040
t4 = 0.25 to 1.00
t13 = 0.0005 to 0.002
t5 = 0.08 to 0.20
t14 = 0.0003 to 0.003
t6 = 0.05 to 0.20
t15 = 0.0005 to 0.003
t7 = 0.05 to 0.20
t16 = 0.000008 to 0.000020
t8 = 0.05 to 0.20
t17 = 0.04 to 0.15
t9 = 0.025 to 0.125
t18 = 0.007 to 0.015
t19 = 0.04 to 0.19
t20 = 0.45 to 0.70
The manufacturing process for constructing the preferred embodiment disclosed in connection with
Next and still referring to
Still referring to
In a second step, electrically conductive bus strips 132a and 132b are printed on first electrically insulative layer 141 as seen at arrow 180 and block 182. In a third step, electrically resistive heating element legs 144 and 145 are thick-film printed and fired on the first electrically insulative layer 141 such that the ends of each leg are printed on and are in electrical communication with the electrically conductive bus strips as seen at arrow 184 and block 186. In a fourth step, an electrically insulative cover layer 142 is thick-film printed and fired over electrically conductive bus 132a, 132b (except at locations of contact pads 62 and 64) and electrically resistive heating element legs 144 and 145, having thickness t13, as seen at arrow 188 and block 190. By way of example and without limitation, thick-film pastes for the [a] first one or more electrically insulative layers 141, [b] second electrically conductive bus strips 132, [c] electrically resistive heating element legs 144 and [d] electrically insulative cover layer 142 may be procured from Heraeus Electronics (Hanau, Germany) or DuPont Microcircuit Materials (Research Triangle Park, North Carolina).
Still referring to
Referring now to
In the discourse that follows, reference is frequently made steps related to a single isothermal cooking plate assembly 50. However, it should be understood that the steps are repeated for each isothermal cooking plate assembly 50 included in a complete griddle system 10 as specified, by way of example, in
Referring now to
Still referring to
While the apparatus, method, and system have been described with reference to various embodiments, those skilled in the art will understand that various changes may be made and equivalents may be substituted for elements thereof without departing from the scope and essence of the disclosure. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the disclosure without departing from the essential scope thereof. Therefore, it is intended that the disclosure not be limited to the particular embodiments disclosed, but that the disclosure will include all embodiments falling within the scope of the appended claims. All citations referred herein are expressly incorporated herein by reference.
Patent | Priority | Assignee | Title |
Patent | Priority | Assignee | Title |
10995959, | Oct 29 2014 | Eggers & Associates, LLC | Isothermal cooking plate apparatus, system, and method of manufacture and use |
6137089, | Jul 15 1996 | U.S. Philips Corporation | Heating element |
6222166, | Aug 09 1999 | Watlow Electric Manufacturing Co. | Aluminum substrate thick film heater |
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